1990
DOI: 10.1007/bf02453036
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On the effective electron mass in quantum well wires of ternary chalcopyrite semiconductors

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Cited by 15 publications
(4 citation statements)
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“…[19]. In the presence of a parallel magnetic field, the modified electron energy spectrum in the quantum well of tetragonal semiconductors can be written as where ~y, +-py ++_ eBd~, 2d~ is the width of the quantum well, 2, 3, ...) is the size quantum number along the x-direction, e is the electron charge, B is the magnetic field along the z-direction which is parallel to the 2D surface (pyp~) of the film, h = h/2r: and h is Planck's constant.…”
Section: -Mathematical Backgroundmentioning
confidence: 97%
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“…[19]. In the presence of a parallel magnetic field, the modified electron energy spectrum in the quantum well of tetragonal semiconductors can be written as where ~y, +-py ++_ eBd~, 2d~ is the width of the quantum well, 2, 3, ...) is the size quantum number along the x-direction, e is the electron charge, B is the magnetic field along the z-direction which is parallel to the 2D surface (pyp~) of the film, h = h/2r: and h is Planck's constant.…”
Section: -Mathematical Backgroundmentioning
confidence: 97%
“…Incorporating the anisotropic crystal potential into the Hamiltonian together with the anisotropic spin-orbit splitting parameters and anisotropic effective electron masses, we have used the dispersion relation of the conduction electrons in bulk specimens of the same semiconductor within the framework of k .p theory [19]. In the absence of crystal field splitting together with the assumptions of isotropic effective electron mass and isotropic spin-orbit splitting parameter, eq.…”
Section: U(~) = (N~ R~/2d~) ~ + K~ + V(d (N~ R:/2d~)mentioning
confidence: 99%
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